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Periodic energy space on an interval

PDF p. 2: §1.2, definition of H¹p(−π,π)

Definition

Assume the Axiom of Choice The Axiom of Choice. By The Axiom of Choice implies countable choice, this implies Countable Choice, as required by the Sobolev interfaces below. Let I=(−π,π) and write H1(I)=W1,2(I;C): its elements are complex L2 equivalence classes whose first weak derivative also belongs to L2(I), equipped with the norm ∥v∥H1(I)=(∥v∥L2(I)2+∥v′∥L2(I)2)1/2 Integer-order Sobolev spaces and their norms. This expression is a well-defined norm by The Sobolev norm descends to equivalence classes, applied with n=1, k=1, p=2 and complex scalars. The periodic energy space is Hp1(−π,π)={v∈H1(I):v∗(−π)=v∗(π)}, with the restricted H1(I) norm. Here v∗ is the unique absolutely continuous representative on [−π,π] of the class v; its endpoint values are the Sobolev traces The trace of a one-dimensional Sobolev function is the pair of endpoint values.

Justification

By The trace of a one-dimensional Sobolev function is the pair of endpoint values, under the stated Axiom of Choice every v∈H1(I) has a uniquely determined absolutely continuous representative on the closed interval, and the endpoint trace map is linear and bounded. Therefore the equality of its endpoint values is independent of the representative of the L2 class. Define D:H1(I)→C by Dv=v∗(−π)−v∗(π). Linearity of the trace gives D(αu+βv)=αDu+βDv for u,v∈H1(I) and α,β∈C. Thus Hp1(−π,π)=ker⁡D is a linear subspace by The kernel and image are linear subspaces, and a linear map is injective if and only if its kernel is trivial; the zero class belongs to it. The norm is well defined by restriction of the Sobolev norm in Integer-order Sobolev spaces and their norms, whose norm axioms and independence of representatives are supplied by The Sobolev norm descends to equivalence classes under Countable Choice, already obtained from the assumed Axiom of Choice.

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